and form a closed algebra with the global conformal generators.The supercurrent in a 2D superconformal field theory is a familiar example of a weight \(h =\frac{3}{2}\)  primary operator that admits a mode decomposition in which the \(\pm \frac{1}{2}\)  modes form a closed subalgebra with the global conformal generators. In gravitational theories, the celestial primary operator weight of \((\frac{3}{2}, \frac{3}{2})\)  can be identified with a particular asymptotic state of the graviton. In Section REF , we explicitly construct this operator as the light transform of a \(\Delta =1\)  conformally soft graviton.This primary was previously discussed in [1]}, [2]}, [3]}, [4]} but not directly constructed with a light transform.
